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Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

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REFERENCES 67<br />

where the sub<strong>in</strong>dices ‘u’ <strong>and</strong> ‘d’ <strong>de</strong>note the mass (M) <strong>and</strong> angular momentum<br />

(J) of the upper <strong>and</strong> lower constituents, respectively, <strong>and</strong> the<br />

constants <strong>and</strong> are <strong>in</strong>troduced <strong>in</strong> the follow<strong>in</strong>g way:<br />

It can be readily proven analytically us<strong>in</strong>g formulas (6) <strong>and</strong> (7) that<br />

<strong>and</strong> cannot assume simultaneously positive values [13], so the<br />

equilibrium of two Kerr black holes possess<strong>in</strong>g positive Komar masses is<br />

impossible. However, the equilibrium states with positive Komar masses<br />

of both constituents are possible when at least one of the constituents is<br />

a superextreme object.<br />

Formulas (4)–(7) give a complete exact solution of the double–Kerr<br />

equilibrium problem.<br />

5. TOWARDS THE ANALYSIS OF THE<br />

MULTI–BLACK<br />

HOLE EQUILIBRIUM STATES<br />

It is very surpris<strong>in</strong>g that although the double–Kerr solution does not<br />

admit equilibrium states of two Kerr black holes, already <strong>in</strong> the case<br />

of three aligned Kerr black holes the gravitational equilibrium is possible<br />

for the constituents with positive Komar masses [14]. The results<br />

recently reported <strong>in</strong> [14] open some new horizons for the study of multi–<br />

black hole equilibrium configurations, <strong>and</strong> one may expect new <strong>in</strong>terest<strong>in</strong>g<br />

future f<strong>in</strong>d<strong>in</strong>gs <strong>in</strong> this area.<br />

Acknowledgments<br />

This work has been partially supported by CONACyT of Mexico<br />

(project 34222–E) <strong>and</strong> by DGICyT of Spa<strong>in</strong> (project PB96-1306).<br />

References<br />

[1] D. Kramer <strong>and</strong> G. Neugebauer, Phys. Lett. A75 (1980) 259.<br />

[2] K. Oohara <strong>and</strong> H. Sato, Prog. Theor. Phys. 66 (1981) 1891.

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